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Successive quasienergy collapse and breakdown of photon blockade in the few-emitter limit

Published 4 Mar 2024 in quant-ph and physics.atom-ph | (2403.02417v2)

Abstract: The emergent behavior that arises in many-body systems of increasing size follows universal laws that become apparent in order-to-disorder transitions. While this behavior has been traditionally studied for large numbers of emitters, recent progress allows for the exploration of the few-emitter limit, where correlations can be measured and connected to microscopic models to gain further insight into order-to-disorder transitions. We explore this few-body limit in the driven and damped Tavis--Cummings model, which describes a collection of atoms interacting with a driven and damped cavity mode. Our exploration revolves around the dressed states of the atomic ensemble and field, whose energies are shown to collapse as the driving field is increased to mark the onset of a dissipative quantum phase transition. The collapse occurs in stages and is an effect of light-matter correlations that are overlooked for single atoms and neglected in mean-field models. The implications of these correlations over the macroscopic observables of the system are presented. We encounter a shift in the expected transition point and an increased number of parity-broken states to choose from once the ordered phase is reached.

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References (3)
  1. R. Gutiérrez-Jáuregui and H. J. Carmichael, Quasienergy collapse in the driven Jaynes–Cummings–Rabi model: correspondence with a charged Dirac particle in an electromagnetic field Phys. Scr. 93 104001 (2018).
  2. H. J. Carmichael Analytical and numerical results for the steady state in cooperative resonance fluorescence J. Phys. B: Atom. Mol. Phys. 13, 3551 (1980).
  3. The dressed state manifolds divide into two kinds depending on the photon number. The first kind occurs for small photon numbers n<na⁢t/2𝑛subscript𝑛𝑎𝑡2n<n_{at}/2italic_n < italic_n start_POSTSUBSCRIPT italic_a italic_t end_POSTSUBSCRIPT / 2 where each manifold contains n+1𝑛1n+1italic_n + 1 states. The second kind occurs for all other photon numbers and each manifold has na⁢t+1subscript𝑛𝑎𝑡1n_{at}+1italic_n start_POSTSUBSCRIPT italic_a italic_t end_POSTSUBSCRIPT + 1 states.
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